Question

Two parallel plates

Equipotential Lines represent for us on a graph the same thing Elevation Lines do for us on a map: They represent a line where the Electric or Gravitational potential is a constant. Maps and voltage graphs have even spacing between values (1V or 500ft or 100m etc)so they can be read easier. These potentials were at 3V, 6V, 9V, 12V, and 15V. In the figure are 5 lines of electric potential drawn from positive charge at left and a negative charge at right.

厶U 15 10 ++/수 25 20 F 2-1331 Science First ㅜ + + + 5 0

a)Draw tiny line segments perpendicular to your equipotential lines. See if you can connect a line segment perpendicular from one equipotential line to another line segment to another equipotential line keeping the ’curve’ needed to attach the two. Then see if you can connect that line to the next.

b) Connect this line to the conductor by making sure it comes perpendicularly out or into the conductor

c) This creates an electric field lined

d) Draw and label at least six electric field lines. Have them be roughly evenly spaced represent different portions of the map.

e) Indicate the direction of the electric field with an arrow on each of your electric field lines.

f) Measure the distance along the electric field “curve” using a string or other method to find the distance the electric field must travel between equipotential lines

g) Now the Electric Field is E=−∆V/∆s where ∆V is your separation of voltage between the two equipotential lines and ∆s is the distance the Electric Field curve traveled.

h) Find the Electric Field for at least 10 points on each map (a good representation of all different points on the map). To ensure as much precision as possible, only consider paths between adjacent equipotential lines. This means ∆V should be the same value for each calculation(your step value of 3V or 2V, etc)

0 0
Add a comment Improve this question Transcribed image text
Answer #1

Question a to e is in this picture:

4 1 10 4. ++ー弋ふ 5 咩绉

h)

−∆V = 3V as the final voltage is smaller than the initial voltage

at point 1, E=−∆V/∆s = -(9-12)/0.016 = 187.5 V/m

2> E=−∆V/∆s = 3/0.02 = 150V/m

3> E=−∆V/∆s = 3/0.021 = 142.85V/m

4> E=−∆V/∆s = 3/0.025= 120V/m

5> E=−∆V/∆s = 3/0.025 = 120V/m

6> E=−∆V/∆s = 3/0.015 = 200V/m

7> E=−∆V/∆s = 3/0.016 = 187.5V/m

8> E=−∆V/∆s = 3/0.015 = 197.3V/m

9> E=−∆V/∆s = 3/0.016 = 187.5 V/m

10> E=−∆V/∆s = 3/0.015= 187.5 V/m

Add a comment
Know the answer?
Add Answer to:
Two parallel plates Equipotential Lines represent for us on a graph the same thing Elevation Line...
Your Answer:

Post as a guest

Your Name:

What's your source?

Earn Coins

Coins can be redeemed for fabulous gifts.

Not the answer you're looking for? Ask your own homework help question. Our experts will answer your question WITHIN MINUTES for Free.
Similar Homework Help Questions
  • A group of students trace out two equipotential surfaces and an electric field line as shown in figure 1.4-1.

    A) Identify the polarity of each terminalB) calculate the electric field for each segment of the electric field line given that the distance between the two digital multi-meter probe tips is 2.0*10^-2 m. C) Determine the potential difference between the two equipotential lines by summing the voltages along the electric field line. Compare this value to the potential difference found by subtracting the voltage of the two equipotential lines. 

  • Q.3 What does figure 5 and figure 6 represent in page 10 in your laboratory manual?...

    Q.3 What does figure 5 and figure 6 represent in page 10 in your laboratory manual? 10 The power source is usually a couple of terminals on the lab table. G represents the galvan The/VVV symbols stand for the resistors in the voltage divider. If there are actually 10 resistors of equal magnitude on your terminal board, as shown in Figure 4, then the voltage across each resistor will be 1/10 of the power supply voltage. You can measure the...

  • Consider a cylindrical capacitor like that shown in Fig. 24.6. Let d = rb − ra...

    Consider a cylindrical capacitor like that shown in Fig. 24.6. Let d = rb − ra be the spacing between the inner and outer conductors. (a) Let the radii of the two conductors be only slightly different, so that d << ra. Show that the result derived in Example 24.4 (Section 24.1) for the capacitance of a cylindrical capacitor then reduces to Eq. (24.2), the equation for the capacitance of a parallel-plate capacitor, with A being the surface area of...

ADVERTISEMENT
Free Homework Help App
Download From Google Play
Scan Your Homework
to Get Instant Free Answers
Need Online Homework Help?
Ask a Question
Get Answers For Free
Most questions answered within 3 hours.
ADVERTISEMENT
ADVERTISEMENT
ADVERTISEMENT